Wednesday, December 7, 2016

Calabi-Yau Manifolds And Worm-Holes

Let us say, that an initially mass-bearing topological substrate -- of which would inherently be of a Calabi-Yau manifold -- is to be altered from its initial tense of a Fourier differentiation as a Hamiltonian operator that is moving via the process of Noether Flow, into being translated into an ensuing tense of a Fourier differentiation as a Hamiltonian operator that is to then be moving via the process of a tachyonic flow, -- over a relatively transient duration of a sequential series of group-related instantons.  Just as the said set of mass-bearing orbifold eigensets that work to comprise the so-stated Calabi-Yau manifold, that is to then travel through the so-eluded-to worm-hole -- the dimensional context of the so-eluded-to metrical-gauge-based Hamiltonian operator will then tend to work to decompactify -- from being of the spatial parameter-related nature of working to bear six or less spatial dimensions plus time (six spatial dimensions that would initially be related to the directly corresponding d-fields, and four spatial dimensions that would initially be related to the directly corresonding f-fields), into next working to bear at least twelve spatial dimensions plus time -- as the overall composite of the said Calabi-Yau manifold is to here be translated as a set of torsional-based indices, that are to here travel through a worm-hole, -- as the said worm-hole is to here work to bend two different Njenhuis-based Gaussian eigensets of mass-bearing topological substrate, in so as to allow for a relatively immediate spatial translation that will here work to inter-bind two relatively far reaches of space in a relatively transient period of time.  Even though a vast portion of the relative speed of a worm-hole is directly related to the contorsioning or the bending of space-time-fabric -- this particular worm-hole of this case is to here bear a certain degree or a certain scalar magnitude of working to bear a tense of a tachyonic propulsion.  This will not disobey the needed tense of Lorentz-Four-Contractions -- since the directly corresponding light-cone-gauge topology of the mass-bearing superstrings that are to here be translated via the so-eluded-to tachyonic-based worm-hole, are to alter from working to bear an inital Kaluza-Klein topology, into then working to bear a Yang-Mills topology.  As the said Calabi-Yau manifold that is to travel through the said worm-hole, is to then be both traveling through twelve or more spatial dimensions, of which it is to tend to change in the number of spatial derivatives that are to equal the number of spatial dimensions that it is traveling through, the worm-hole will tend to always -- at the critical cusps of the bending of space via the worm-hole -- change in more derivatives than the number of spatial dimensions that it is moving through.  This will then mean that any Calabi-Yau manifold that is to travel through a worm-hole, will tend to not be Yau-Exact at the critical cusps of the contorsioning of space, where the directly corresponding bending of space is to here be relatively maximized, as a Hamiltonian operand by which the said Calabi-Yau manifold is to here be Yukawa to it, as it is being translated in such a tachyonic manner.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

No comments: